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Professor Diablo wants to say something
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# %% | ||
# + | ||
## Mesh refinement ... | ||
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# to fix trame issue | ||
import nest_asyncio | ||
nest_asyncio.apply() | ||
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import os | ||
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os.environ["UW_TIMING_ENABLE"] = "1" | ||
os.environ["SYMPY_USE_CACHE"] = "no" | ||
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import petsc4py | ||
from petsc4py import PETSc | ||
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from underworld3 import timing | ||
from underworld3 import adaptivity | ||
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import underworld3 as uw | ||
from underworld3 import function | ||
from enum import Enum | ||
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import numpy as np | ||
import sympy | ||
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# %% | ||
class bd(Enum): | ||
Upper=2 | ||
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batmesh = uw.discretisation.Mesh( | ||
"Batmesh_number_one.h5", | ||
coordinate_system_type=uw.coordinates.CoordinateSystemType.CYLINDRICAL2D, | ||
boundaries=bd) | ||
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# %% | ||
batmesh.dm.view() | ||
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# %% | ||
Rayleigh_number = uw.function.expression(r"\textrm{Ra}", sympy.sympify(10)**6, "Rayleigh number") | ||
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# %% | ||
v_soln = uw.discretisation.MeshVariable("U", batmesh, batmesh.dim, degree=2, continuous=True) | ||
p_soln = uw.discretisation.MeshVariable("P", batmesh, 1, degree=1, continuous=True) | ||
t_soln = uw.discretisation.MeshVariable("T", batmesh, 1, degree=2) | ||
cell_properties = uw.discretisation.MeshVariable("Bat", batmesh, 1, degree=0) | ||
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# %% | ||
cell_properties.read_timestep( | ||
"Batmesh_cell_properties", | ||
data_name="L", | ||
index=0, | ||
) | ||
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# %% | ||
# Create Stokes object | ||
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stokes = uw.systems.Stokes( | ||
batmesh, | ||
velocityField=v_soln, | ||
pressureField=p_soln, | ||
) | ||
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# Constant viscosity | ||
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stokes.constitutive_model = uw.constitutive_models.ViscousFlowModel | ||
stokes.constitutive_model.Parameters.shear_viscosity_0 = 1 | ||
stokes.tolerance = 1.0e-3 | ||
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unit_r_vec = batmesh.CoordinateSystem.unit_e_0 | ||
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# free slip. | ||
# note with petsc we always need to provide a vector of correct cardinality. | ||
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stokes.add_natural_bc(10000 * unit_r_vec.dot(v_soln.sym) * unit_r_vec, "Upper") | ||
stokes.bodyforce = Rayleigh_number * unit_r_vec * t_soln.sym[0] | ||
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# Make the bat stagnant | ||
# stokes.bodyforce -= 10000 * (1-cell_properties.sym[0]) * v_soln.sym | ||
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stokes.view() | ||
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# %% | ||
adv_diff = uw.systems.AdvDiffusionSLCN( | ||
batmesh, | ||
u_Field=t_soln, | ||
V_fn=v_soln, | ||
) | ||
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adv_diff.constitutive_model = uw.constitutive_models.DiffusionModel | ||
adv_diff.constitutive_model.Parameters.diffusivity = 1 | ||
adv_diff.f = 10 * (1-cell_properties.sym[0]) | ||
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adv_diff.add_dirichlet_bc(0.0, "Upper") | ||
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t_init = 1-cell_properties.sym[0] | ||
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with batmesh.access(t_soln): | ||
t_soln.data[:,0] = uw.function.evalf(t_init, t_soln.coords) | ||
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# %% | ||
stokes.solve(zero_init_guess=True) | ||
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# %% | ||
v_soln.view() | ||
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# %% | ||
t_step = 0 | ||
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# %% | ||
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for step in range(0, 50): | ||
stokes.solve(zero_init_guess=False) | ||
delta_t = 2.0 * stokes.estimate_dt() | ||
adv_diff.solve(timestep=delta_t, zero_init_guess=False) | ||
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# stats then loop | ||
tstats = t_soln.stats() | ||
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if uw.mpi.rank == 0: | ||
print("Timestep {}, dt {}".format(step, delta_t)) | ||
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batmesh.write_timestep( | ||
"Batmesh", | ||
meshUpdates=True, | ||
meshVars=[p_soln, v_soln, t_soln], | ||
outputPath="output", | ||
index=t_step, | ||
) | ||
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with batmesh.access(t_soln): | ||
t_soln.data[:,0] = np.maximum(t_soln.data[:,0], uw.function.evalf(t_init, t_soln.coords)) | ||
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t_step += 1 | ||
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# %% | ||
if uw.mpi.size == 1: | ||
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import pyvista as pv | ||
import underworld3.visualisation as vis | ||
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pvmesh = vis.mesh_to_pv_mesh(batmesh) | ||
pvmesh.point_data["T"] = vis.scalar_fn_to_pv_points(pvmesh, t_soln.sym[0]) | ||
pvmesh.point_data["V"] = vis.vector_fn_to_pv_points(pvmesh, v_soln.sym) | ||
pvmesh.point_data["L"] = vis.scalar_fn_to_pv_points(pvmesh, cell_properties.sym[0]) | ||
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pl = pv.Plotter(window_size=(750, 750)) | ||
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pvstream = pvmesh.streamlines_from_source( | ||
pvmesh.cell_centers(), | ||
vectors="V", | ||
integrator_type=45, | ||
surface_streamlines=True, | ||
max_steps=1000, | ||
max_time=0.25, | ||
) | ||
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pl.add_mesh( | ||
pvmesh, | ||
cmap="Oranges", | ||
scalars="T", | ||
edge_color="Grey", | ||
show_edges=False, | ||
use_transparency=False, | ||
opacity=1.0, | ||
show_scalar_bar=True, | ||
clim=[0,1] | ||
) | ||
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pl.add_mesh( | ||
pvmesh, | ||
scalars="L", | ||
cmap="Greys_r", | ||
edge_color="Black", | ||
opacity="L", | ||
show_edges=False, | ||
use_transparency=True, | ||
show_scalar_bar=False, | ||
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) | ||
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# pl.add_mesh(pvstream, cmap="jet", show_scalar_bar=False) | ||
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# pl.add_arrows(pvmesh.points, pvmesh.point_data["V"], | ||
# mag=float(20.0/Rayleigh_number.sym), | ||
# show_scalar_bar=False) | ||
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pl.show(jupyter_backend='html') | ||
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# %% | ||
## Check the results saved to file | ||
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expt_name = "Batmesh" | ||
output_path="output" | ||
step = 20 | ||
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v_soln.read_timestep(expt_name, "U", step, outputPath=output_path) | ||
p_soln.read_timestep(expt_name, "P", step, outputPath=output_path) | ||
t_soln.read_timestep(expt_name, "T", step, outputPath=output_path) | ||
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# %% | ||
adv_diff | ||
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# %% |
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